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| .. _custom_metal_kernels: | |
| Custom Metal Kernels | |
| ==================== | |
| MLX supports writing custom Metal kernels through the Python and C++ APIs. | |
| Simple Example | |
| -------------- | |
| .. currentmodule:: mlx.core | |
| Let's write a custom kernel that computes ``exp`` elementwise: | |
| .. code-block:: python | |
| source = """ | |
| uint elem = thread_position_in_grid.x; | |
| T tmp = inp[elem]; | |
| out[elem] = metal::exp(tmp); | |
| """ | |
| kernel = mx.fast.metal_kernel( | |
| name="myexp", | |
| input_names=["inp"], | |
| output_names=["out"], | |
| source=source, | |
| ) | |
| def exp_elementwise(a: mx.array): | |
| outputs = kernel( | |
| inputs=[a], | |
| template=[("T", mx.float32)], | |
| grid=(a.size, 1, 1), | |
| threadgroup=(256, 1, 1), | |
| output_shapes=[a.shape], | |
| output_dtypes=[a.dtype], | |
| ) | |
| return outputs[0] | |
| a = mx.random.normal(shape=(4, 16)).astype(mx.float16) | |
| b = exp_elementwise(a) | |
| assert mx.allclose(b, mx.exp(a)) | |
| Every time you make a kernel, a new Metal library is created and possibly | |
| JIT compiled. To reduce the overhead from that, build the kernel once with | |
| :func:`fast.metal_kernel` and then use it many times. | |
| .. note:: | |
| Only pass the body of the Metal kernel in ``source``. The function | |
| signature is generated automatically. | |
| The full function signature will be generated using: | |
| * The shapes/dtypes of ``inputs`` | |
| In the above, ``a`` is an ``mx.array`` of type ``mx.float16`` and we pass it with the key ``inp`` | |
| so we will add ``const device float16_t* inp`` to the signature. | |
| ``inp_shape``, ``inp_strides`` and ``inp_ndim`` are also added for convenience if they are present | |
| in ``source``. | |
| * The list of ``output_dtypes`` | |
| In the above, ``out`` is an ``mx.array`` of type ``mx.float16`` | |
| so we add ``device float16_t* out``. | |
| * Template parameters passed using ``template`` | |
| In the above, ``template=[("T", mx.float32)]`` adds a template of ``template <typename T>`` to the function | |
| and instantiates the template with ``custom_kernel_myexp_float<float>``. | |
| Template parameters can be ``mx.core.Dtype``, ``int`` or ``bool``. | |
| * Metal attributes used in ``source`` such as ``[[thread_position_in_grid]]`` | |
| These will be added as function arguments. | |
| All the attributes defined in Table 5.8 of the `Metal Shading Language Specification <https://developer.apple.com/metal/Metal-Shading-Language-Specification.pdf>`_ are supported. | |
| Putting this all together, the generated function signature for ``myexp`` is as follows: | |
| .. code-block:: cpp | |
| template <typename T> | |
| [[kernel]] void custom_kernel_myexp_float( | |
| const device float16_t* inp [[buffer(0)]], | |
| device float16_t* out [[buffer(1)]], | |
| uint3 thread_position_in_grid [[thread_position_in_grid]]) { | |
| uint elem = thread_position_in_grid.x; | |
| T tmp = inp[elem]; | |
| out[elem] = metal::exp(tmp); | |
| } | |
| template [[host_name("custom_kernel_myexp_float")]] [[kernel]] decltype(custom_kernel_myexp_float<float>) custom_kernel_myexp_float<float>; | |
| Note: ``grid`` and ``threadgroup`` are parameters to the Metal `dispatchThreads | |
| <https://developer.apple.com/documentation/metal/mtlcomputecommandencoder/2866532-dispatchthreads>`_ | |
| function. This means we will launch ``mx.prod(grid)`` threads, subdivided into | |
| ``threadgroup`` size threadgroups. For optimal performance, each thread group | |
| dimension should be less than or equal to the corresponding grid dimension. | |
| Passing ``verbose=True`` to :func:`ast.metal_kernel.__call__` will print the | |
| generated code for debugging purposes. | |
| Using Shape/Strides | |
| ------------------- | |
| :func:`fast.metal_kernel` supports an argument ``ensure_row_contiguous`` which | |
| is ``True`` by default. This will copy the array inputs if needed | |
| before the kernel is launched to ensure that the memory layout is row | |
| contiguous. Generally this makes writing the kernel easier, since we don't | |
| have to worry about gaps or the ordering of the dims when indexing. | |
| If we want to avoid this copy, :func:`fast.metal_kernel` automatically passes | |
| ``a_shape``, ``a_strides`` and ``a_ndim`` for each input array ``a`` if any are | |
| present in ``source``. We can then use MLX's built in indexing utils to fetch | |
| the right elements for each thread. | |
| Let's convert ``myexp`` above to support arbitrarily strided arrays without | |
| relying on a copy from ``ensure_row_contiguous``: | |
| .. code-block:: python | |
| source = """ | |
| uint elem = thread_position_in_grid.x; | |
| // Utils from `mlx/backend/metal/kernels/utils.h` are automatically included | |
| uint loc = elem_to_loc(elem, inp_shape, inp_strides, inp_ndim); | |
| T tmp = inp[loc]; | |
| // Output arrays are always row contiguous | |
| out[elem] = metal::exp(tmp); | |
| """ | |
| kernel = mx.fast.metal_kernel( | |
| name="myexp_strided", | |
| input_names=["inp"], | |
| output_names=["out"], | |
| source=source, | |
| ensure_row_contiguous=False, | |
| ) | |
| def exp_elementwise(a: mx.array): | |
| outputs = kernel( | |
| inputs=[a], | |
| template=[("T", mx.float32)], | |
| grid=(a.size, 1, 1), | |
| threadgroup=(256, 1, 1), | |
| output_shapes=[a.shape], | |
| output_dtypes=[a.dtype], | |
| ) | |
| return outputs[0] | |
| a = mx.random.normal(shape=(4, 16)).astype(mx.float16) | |
| # make non-contiguous | |
| a = a[::2] | |
| b = exp_elementwise(a) | |
| assert mx.allclose(b, mx.exp(a)) | |
| Complex Example | |
| ----------------------------- | |
| Let's implement a more complex example: ``grid_sample`` in ``"bilinear"`` mode. | |
| We'll start with the following MLX implementation using standard ops: | |
| .. code-block:: python | |
| def grid_sample_ref(x, grid): | |
| N, H_in, W_in, _ = x.shape | |
| ix = ((grid[..., 0] + 1) * W_in - 1) / 2 | |
| iy = ((grid[..., 1] + 1) * H_in - 1) / 2 | |
| ix_nw = mx.floor(ix).astype(mx.int32) | |
| iy_nw = mx.floor(iy).astype(mx.int32) | |
| ix_ne = ix_nw + 1 | |
| iy_ne = iy_nw | |
| ix_sw = ix_nw | |
| iy_sw = iy_nw + 1 | |
| ix_se = ix_nw + 1 | |
| iy_se = iy_nw + 1 | |
| nw = (ix_se - ix) * (iy_se - iy) | |
| ne = (ix - ix_sw) * (iy_sw - iy) | |
| sw = (ix_ne - ix) * (iy - iy_ne) | |
| se = (ix - ix_nw) * (iy - iy_nw) | |
| I_nw = x[mx.arange(N)[:, None, None], iy_nw, ix_nw, :] | |
| I_ne = x[mx.arange(N)[:, None, None], iy_ne, ix_ne, :] | |
| I_sw = x[mx.arange(N)[:, None, None], iy_sw, ix_sw, :] | |
| I_se = x[mx.arange(N)[:, None, None], iy_se, ix_se, :] | |
| mask_nw = (iy_nw >= 0) & (iy_nw <= H_in - 1) & (ix_nw >= 0) & (ix_nw <= W_in - 1) | |
| mask_ne = (iy_ne >= 0) & (iy_ne <= H_in - 1) & (ix_ne >= 0) & (ix_ne <= W_in - 1) | |
| mask_sw = (iy_sw >= 0) & (iy_sw <= H_in - 1) & (ix_sw >= 0) & (ix_sw <= W_in - 1) | |
| mask_se = (iy_se >= 0) & (iy_se <= H_in - 1) & (ix_se >= 0) & (ix_se <= W_in - 1) | |
| I_nw *= mask_nw[..., None] | |
| I_ne *= mask_ne[..., None] | |
| I_sw *= mask_sw[..., None] | |
| I_se *= mask_se[..., None] | |
| output = nw[..., None] * I_nw + ne[..., None] * I_ne + sw[..., None] * I_sw + se[..., None] * I_se | |
| return output | |
| Now let's use :func:`custom_function` together with :func:`fast.metal_kernel` | |
| to write a fast GPU kernel for both the forward and backward passes. | |
| First we'll implement the forward pass as a fused kernel: | |
| .. code-block:: python | |
| source = """ | |
| uint elem = thread_position_in_grid.x; | |
| int H = x_shape[1]; | |
| int W = x_shape[2]; | |
| int C = x_shape[3]; | |
| int gH = grid_shape[1]; | |
| int gW = grid_shape[2]; | |
| int w_stride = C; | |
| int h_stride = W * w_stride; | |
| int b_stride = H * h_stride; | |
| uint grid_idx = elem / C * 2; | |
| float ix = ((grid[grid_idx] + 1) * W - 1) / 2; | |
| float iy = ((grid[grid_idx + 1] + 1) * H - 1) / 2; | |
| int ix_nw = floor(ix); | |
| int iy_nw = floor(iy); | |
| int ix_ne = ix_nw + 1; | |
| int iy_ne = iy_nw; | |
| int ix_sw = ix_nw; | |
| int iy_sw = iy_nw + 1; | |
| int ix_se = ix_nw + 1; | |
| int iy_se = iy_nw + 1; | |
| T nw = (ix_se - ix) * (iy_se - iy); | |
| T ne = (ix - ix_sw) * (iy_sw - iy); | |
| T sw = (ix_ne - ix) * (iy - iy_ne); | |
| T se = (ix - ix_nw) * (iy - iy_nw); | |
| int batch_idx = elem / C / gH / gW * b_stride; | |
| int channel_idx = elem % C; | |
| int base_idx = batch_idx + channel_idx; | |
| T I_nw = x[base_idx + iy_nw * h_stride + ix_nw * w_stride]; | |
| T I_ne = x[base_idx + iy_ne * h_stride + ix_ne * w_stride]; | |
| T I_sw = x[base_idx + iy_sw * h_stride + ix_sw * w_stride]; | |
| T I_se = x[base_idx + iy_se * h_stride + ix_se * w_stride]; | |
| I_nw = iy_nw >= 0 && iy_nw <= H - 1 && ix_nw >= 0 && ix_nw <= W - 1 ? I_nw : 0; | |
| I_ne = iy_ne >= 0 && iy_ne <= H - 1 && ix_ne >= 0 && ix_ne <= W - 1 ? I_ne : 0; | |
| I_sw = iy_sw >= 0 && iy_sw <= H - 1 && ix_sw >= 0 && ix_sw <= W - 1 ? I_sw : 0; | |
| I_se = iy_se >= 0 && iy_se <= H - 1 && ix_se >= 0 && ix_se <= W - 1 ? I_se : 0; | |
| out[elem] = nw * I_nw + ne * I_ne + sw * I_sw + se * I_se; | |
| """ | |
| kernel = mx.fast.metal_kernel( | |
| name="grid_sample", | |
| input_names=["x", "grid"], | |
| output_names=["out"], | |
| source=source, | |
| ) | |
| .custom_function | |
| def grid_sample(x, grid): | |
| assert x.ndim == 4, "`x` must be 4D." | |
| assert grid.ndim == 4, "`grid` must be 4D." | |
| B, _, _, C = x.shape | |
| _, gN, gM, D = grid.shape | |
| out_shape = (B, gN, gM, C) | |
| assert D == 2, "Last dim of `grid` must be size 2." | |
| outputs = kernel( | |
| inputs=[x, grid], | |
| template=[("T", x.dtype)], | |
| output_shapes=[out_shape], | |
| output_dtypes=[x.dtype], | |
| grid=(np.prod(out_shape), 1, 1), | |
| threadgroup=(256, 1, 1), | |
| ) | |
| return outputs[0] | |
| For a reasonably sized input such as: | |
| .. code-block:: python | |
| x.shape = (8, 1024, 1024, 64) | |
| grid.shape = (8, 256, 256, 2) | |
| On an M1 Max, we see a big performance improvement: | |
| ``55.7ms -> 6.7ms => 8x speed up`` | |
| Grid Sample VJP | |
| --------------- | |
| Since we decorated ``grid_sample`` with :func:`custom_function`, we can now | |
| define its custom vjp transform so MLX can differentiate it. | |
| The backwards pass requires atomically updating ``x_grad``/``grid_grad`` and so | |
| requires a few extra :func:`fast.metal_kernel` features: | |
| * ``init_value=0`` | |
| Initialize all of the kernel's outputs to this value before it runs. This allows us to update only part of the output arrays with the kernel. | |
| * ``atomic_outputs=True`` | |
| Designate all of the kernel outputs as ``atomic`` in the function signature. | |
| This means we can use Metal's ``atomic`` features to simultaneously update the ``x_grad`` and ``grid_grad`` arrays from multiple threadgroups. | |
| See section 6.15 of the `Metal Shading Language Specification <https://developer.apple.com/metal/Metal-Shading-Language-Specification.pdf>`_ for more details. | |
| We can then implement the backwards pass as follows: | |
| .. code-block:: python | |
| source = """ | |
| uint elem = thread_position_in_grid.x; | |
| int H = x_shape[1]; | |
| int W = x_shape[2]; | |
| int C = x_shape[3]; | |
| // Pad C to the nearest larger simdgroup size multiple | |
| int C_padded = ceildiv(C, threads_per_simdgroup) * threads_per_simdgroup; | |
| int gH = grid_shape[1]; | |
| int gW = grid_shape[2]; | |
| int w_stride = C; | |
| int h_stride = W * w_stride; | |
| int b_stride = H * h_stride; | |
| uint grid_idx = elem / C_padded * 2; | |
| float ix = ((grid[grid_idx] + 1) * W - 1) / 2; | |
| float iy = ((grid[grid_idx + 1] + 1) * H - 1) / 2; | |
| int ix_nw = floor(ix); | |
| int iy_nw = floor(iy); | |
| int ix_ne = ix_nw + 1; | |
| int iy_ne = iy_nw; | |
| int ix_sw = ix_nw; | |
| int iy_sw = iy_nw + 1; | |
| int ix_se = ix_nw + 1; | |
| int iy_se = iy_nw + 1; | |
| T nw = (ix_se - ix) * (iy_se - iy); | |
| T ne = (ix - ix_sw) * (iy_sw - iy); | |
| T sw = (ix_ne - ix) * (iy - iy_ne); | |
| T se = (ix - ix_nw) * (iy - iy_nw); | |
| int batch_idx = elem / C_padded / gH / gW * b_stride; | |
| int channel_idx = elem % C_padded; | |
| int base_idx = batch_idx + channel_idx; | |
| T gix = T(0); | |
| T giy = T(0); | |
| if (channel_idx < C) { | |
| int cot_index = elem / C_padded * C + channel_idx; | |
| T cot = cotangent[cot_index]; | |
| if (iy_nw >= 0 && iy_nw <= H - 1 && ix_nw >= 0 && ix_nw <= W - 1) { | |
| int offset = base_idx + iy_nw * h_stride + ix_nw * w_stride; | |
| atomic_fetch_add_explicit(&x_grad[offset], nw * cot, memory_order_relaxed); | |
| T I_nw = x[offset]; | |
| gix -= I_nw * (iy_se - iy) * cot; | |
| giy -= I_nw * (ix_se - ix) * cot; | |
| } | |
| if (iy_ne >= 0 && iy_ne <= H - 1 && ix_ne >= 0 && ix_ne <= W - 1) { | |
| int offset = base_idx + iy_ne * h_stride + ix_ne * w_stride; | |
| atomic_fetch_add_explicit(&x_grad[offset], ne * cot, memory_order_relaxed); | |
| T I_ne = x[offset]; | |
| gix += I_ne * (iy_sw - iy) * cot; | |
| giy -= I_ne * (ix - ix_sw) * cot; | |
| } | |
| if (iy_sw >= 0 && iy_sw <= H - 1 && ix_sw >= 0 && ix_sw <= W - 1) { | |
| int offset = base_idx + iy_sw * h_stride + ix_sw * w_stride; | |
| atomic_fetch_add_explicit(&x_grad[offset], sw * cot, memory_order_relaxed); | |
| T I_sw = x[offset]; | |
| gix -= I_sw * (iy - iy_ne) * cot; | |
| giy += I_sw * (ix_ne - ix) * cot; | |
| } | |
| if (iy_se >= 0 && iy_se <= H - 1 && ix_se >= 0 && ix_se <= W - 1) { | |
| int offset = base_idx + iy_se * h_stride + ix_se * w_stride; | |
| atomic_fetch_add_explicit(&x_grad[offset], se * cot, memory_order_relaxed); | |
| T I_se = x[offset]; | |
| gix += I_se * (iy - iy_nw) * cot; | |
| giy += I_se * (ix - ix_nw) * cot; | |
| } | |
| } | |
| T gix_mult = W / 2; | |
| T giy_mult = H / 2; | |
| // Reduce across each simdgroup first. | |
| // This is much faster than relying purely on atomics. | |
| gix = simd_sum(gix); | |
| giy = simd_sum(giy); | |
| if (thread_index_in_simdgroup == 0) { | |
| atomic_fetch_add_explicit(&grid_grad[grid_idx], gix * gix_mult, memory_order_relaxed); | |
| atomic_fetch_add_explicit(&grid_grad[grid_idx + 1], giy * giy_mult, memory_order_relaxed); | |
| } | |
| """ | |
| kernel = mx.fast.metal_kernel( | |
| name="grid_sample_grad", | |
| input_names=["x", "grid", "cotangent"], | |
| output_names=["x_grad", "grid_grad"], | |
| source=source, | |
| atomic_outputs=True, | |
| ) | |
| .vjp | |
| def grid_sample_vjp(primals, cotangent, _): | |
| x, grid = primals | |
| B, _, _, C = x.shape | |
| _, gN, gM, D = grid.shape | |
| assert D == 2, "Last dim of `grid` must be size 2." | |
| # pad the output channels to simd group size | |
| # so that our `simd_sum`s don't overlap. | |
| simdgroup_size = 32 | |
| C_padded = (C + simdgroup_size - 1) // simdgroup_size * simdgroup_size | |
| grid_size = B * gN * gM * C_padded | |
| outputs = kernel( | |
| inputs=[x, grid, cotangent], | |
| template=[("T", x.dtype)], | |
| output_shapes=[x.shape, grid.shape], | |
| output_dtypes=[x.dtype, x.dtype], | |
| grid=(grid_size, 1, 1), | |
| threadgroup=(256, 1, 1), | |
| init_value=0, | |
| ) | |
| return outputs[0], outputs[1] | |
| There's an even larger speed up for the vjp: | |
| ``676.4ms -> 16.7ms => 40x speed up`` | |